JP2000321161A - Capacitive vacuum sensor - Google Patents
Capacitive vacuum sensorInfo
- Publication number
- JP2000321161A JP2000321161A JP11134136A JP13413699A JP2000321161A JP 2000321161 A JP2000321161 A JP 2000321161A JP 11134136 A JP11134136 A JP 11134136A JP 13413699 A JP13413699 A JP 13413699A JP 2000321161 A JP2000321161 A JP 2000321161A
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- Prior art keywords
- electrode
- diaphragm
- sensor
- substrate
- temperature
- Prior art date
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Abstract
(57)【要約】
【課題】 本発明は、温度変化に起因する測定誤差を抑
え、センサの測定精度を向上させることを目的としたも
のである。
【解決手段】 本発明は内部に空間を隔てて対向する一
対のダイヤフラム電極と固定電極とを基板に配置し、前
記ダイヤフラム電極と対向する固定電極との間の静電容
量の変化から圧力を測定する真空センサにおいて、前記
ダイヤフラム電極および前記固定電極が配置されている
前記基板上にダイヤフラム電極周辺を一定温度にする為
の温度制御手段を設けると共に、前記真空センサの圧力
検出部を線材で支持したことを特徴とする静電容量型真
空センサとすることにより、課題を解決したのである。
(57) [Problem] An object of the present invention is to suppress a measurement error due to a temperature change and improve the measurement accuracy of a sensor. According to the present invention, a pair of diaphragm electrodes and a fixed electrode facing each other with a space therebetween are disposed on a substrate, and pressure is measured from a change in capacitance between the diaphragm electrode and the fixed electrode facing the same. In the vacuum sensor, a temperature control unit for maintaining a constant temperature around the diaphragm electrode is provided on the substrate on which the diaphragm electrode and the fixed electrode are arranged, and a pressure detecting unit of the vacuum sensor is supported by a wire. The problem was solved by using a capacitance type vacuum sensor characterized by the above.
Description
【0001】[0001]
【発明の属する技術分野】この発明は、温度変化に起因
する測定誤差を抑え、センサの測定精度を向上させるこ
とを目的とした静電容量型真空センサに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a capacitance type vacuum sensor for suppressing a measurement error caused by a temperature change and improving a measurement accuracy of the sensor.
【0002】[0002]
【従来の技術】電子部品や半導体製品を製造する過程に
おいては、真空装置内で薄膜を形成したりあるいはエッ
チングするプロセスは不可欠である。この際に、真空装
置内圧力は、一定に保たれながらプロセスが進められる
のが普通であるが、真空装置内の圧力測定手段として
は、静電容量型真空センサがしばしば用いられる。図2
に従来の温度制御機能付き静電容量型真空センサの一例
を示す。静電容量型真空センサは、センサ内部に基準圧
力となる部屋(基準圧力室1)を設け、この基準圧力室
1は、真空装置2に連通する領域3とダイヤフラム電極
4で仕切られており、このダイヤフラム電極4(弾性隔
膜)に対向して固定電極5が配置されている。前記基準
圧力室1と真空装置2に連通する領域3との間に圧力差
があるとダイヤフラム電極4は圧力差に応じて変位する
が、ダイヤフラム電極4と固定電極5間の静電容量は両
者の距離に反比例するので、導線9を通してこれらの電
気情報を電気回路7に伝え、静電容量を電圧あるいは電
流に変換してセンサ外に出力することで圧力を測定する
ことができる。しかしながら、ダイヤフラム電極4が変
位する要因は、真空装置内の圧力だけではなく、ダイヤ
フラム電極4とその周辺材料の熱膨張係数が異なるため
に、センサの温度変化とともにダイヤフラム電極4に微
量な変位が生じ、圧力測定に誤差を発生させる。そこ
で、従来の高精度型の静電容量型真空センサは、内部に
加熱部6を設け、センサ温度を一定に保ちながら温度変
化に起因する測定誤差を防いでいるが、加熱部6はダイ
ヤフラム電極4及び固定電極5を包括するように外側か
ら加熱し、固定電極5近傍に設置した温度測定部8によ
り温度を測定し、センサ内部全体を一定温度に保つ構造
となっている。また、加熱部6の外側には断熱材10を
配置し、加熱部6の熱がセンサケース11へ伝導して高
温になるのを防いでいる。2. Description of the Related Art In the process of manufacturing electronic parts and semiconductor products, a process of forming or etching a thin film in a vacuum apparatus is indispensable. At this time, the process is usually performed while the pressure in the vacuum device is kept constant, but a capacitance type vacuum sensor is often used as a pressure measuring means in the vacuum device. FIG.
FIG. 1 shows an example of a conventional capacitive vacuum sensor with a temperature control function. The capacitance-type vacuum sensor has a chamber (reference pressure chamber 1) having a reference pressure inside the sensor, and the reference pressure chamber 1 is partitioned by a region 3 communicating with a vacuum device 2 and a diaphragm electrode 4. A fixed electrode 5 is arranged to face the diaphragm electrode 4 (elastic diaphragm). If there is a pressure difference between the reference pressure chamber 1 and the region 3 communicating with the vacuum device 2, the diaphragm electrode 4 is displaced in accordance with the pressure difference, but the capacitance between the diaphragm electrode 4 and the fixed electrode 5 , The electric information is transmitted to the electric circuit 7 through the conducting wire 9, the capacitance is converted into a voltage or a current, and output to the outside of the sensor, so that the pressure can be measured. However, because the diaphragm electrode 4 is displaced not only by the pressure in the vacuum device but also by the difference in the thermal expansion coefficients of the diaphragm electrode 4 and the surrounding materials, a slight displacement occurs in the diaphragm electrode 4 with a change in the temperature of the sensor. , Causing errors in pressure measurements. Therefore, in the conventional high-precision capacitive vacuum sensor, a heating unit 6 is provided inside to prevent a measurement error due to a temperature change while keeping the sensor temperature constant. However, the heating unit 6 has a diaphragm electrode. 4 and the fixed electrode 5 are heated from the outside so as to cover them, the temperature is measured by a temperature measuring unit 8 installed near the fixed electrode 5, and the whole inside of the sensor is kept at a constant temperature. A heat insulating material 10 is arranged outside the heating unit 6 to prevent heat of the heating unit 6 from being conducted to the sensor case 11 and becoming high in temperature.
【0003】[0003]
【発明が解決しようとする課題】静電容量型真空センサ
の温度変化に起因する測定誤差を抑える手段として、セ
ンサ内部を一定温度に加熱・保存することによりセンサ
の測定精度は向上した。原理的には、センサ内部のダイ
ヤフラム電極(弾性隔膜)と固定電極、そしてそれらを
支えている支持部のみを均一に加熱・保温し、周辺温度
の変化がこれらの部分の機械的変形に影響を及ぼさない
ようにすれば温度変化による測定誤差の問題は解決する
ことができる。しかしながら、前記従来の真空センサで
は、これらのダイヤフラム電極(弾性隔膜)や固定電極
は機械的加工によって製造されるために小型化や複雑な
形状の加工が難しく、したがって、これらの大きい部品
を均一の温度に加熱・保温するためにはこれらを全体的
に包み込むように加熱手段を配置して外部から加熱する
必要がある。その結果、被加熱部の熱容量が大きくなる
ために昇温時間が長くなり、またセンサ温度を一定に制
御している状態でも、センサの急激な温度変化に対して
即反応することができない問題点があり、また安定した
圧力測定ができるまでに数時間かかり、そのために多く
の時間と電力を費す問題点があった。As a means for suppressing a measurement error due to a temperature change of the capacitance type vacuum sensor, the measurement accuracy of the sensor has been improved by heating and storing the inside of the sensor at a constant temperature. In principle, only the diaphragm electrode (elastic diaphragm) and fixed electrode inside the sensor and the supporting part that supports them are heated and kept uniformly, and the change in ambient temperature affects the mechanical deformation of these parts. If it does not, the problem of measurement error due to temperature change can be solved. However, in the conventional vacuum sensor, since these diaphragm electrodes (elastic diaphragms) and fixed electrodes are manufactured by mechanical processing, miniaturization and processing of complicated shapes are difficult. In order to heat and maintain the temperature, it is necessary to arrange a heating means so as to entirely cover them and to heat them from the outside. As a result, there is a problem that the heat capacity of the heated portion is increased, so that the temperature rise time becomes longer, and even when the sensor temperature is controlled to be constant, it is not possible to immediately respond to a sudden temperature change of the sensor. In addition, it takes several hours until a stable pressure measurement can be performed, so that much time and power are required.
【0004】[0004]
【課題を解決するための手段】本発明は熱容量の小さい
導電性薄膜からなるダイヤフラム電極を基板に固定して
固定電極に対向させると共に、前記ダイヤフラム電極の
周辺を一定温度に制御すべく温度制御手段を設けること
により前記従来の問題点を解決したのである。According to the present invention, there is provided a temperature control means for fixing a diaphragm electrode made of a conductive thin film having a small heat capacity to a substrate so as to face the fixed electrode and controlling the periphery of the diaphragm electrode to a constant temperature. Is provided to solve the above-mentioned conventional problem.
【0005】即ち本発明は内部に空間を隔てて対向する
一対のダイヤフラム電極と固定電極とを基板に配置し、
前記ダイヤフラム電極と対向する固定電極との間の静電
容量の変化から圧力を測定する真空センサにおいて、前
記ダイヤフラム電極および前記固定電極が配置されてい
る前記基板上にダイヤフラム電極周辺を一定温度にする
為の温度制御手段を設けたことを特徴とする静電容量型
真空センサである。また、他の発明は内部に空間を隔て
て対向する一対のダイヤフラム電極と固定電極とを基板
に配置し、前記ダイヤフラム電極と対向する固定電極と
の間の静電容量の変化から圧力を測定する真空センサに
おいて、前記ダイヤフラム電極および前記固定電極が配
置されている前記基板上にダイヤフラム電極周辺を一定
温度にする為の温度制御手段を設けると共に、前記真空
センサの圧力検出部を複数本の線材で支持したことを特
徴とする静電容量型真空センサである。前記において、
温度制御手段は、基板上に発熱層と温度測定層を形成し
たものである。That is, according to the present invention, a pair of diaphragm electrodes and a fixed electrode facing each other with a space therebetween are arranged on a substrate,
In a vacuum sensor that measures pressure from a change in capacitance between the diaphragm electrode and an opposing fixed electrode, a constant temperature is maintained around the diaphragm electrode on the substrate on which the diaphragm electrode and the fixed electrode are arranged. A capacitance type vacuum sensor provided with a temperature control means for the same. In another invention, a pair of a diaphragm electrode and a fixed electrode opposed to each other with a space inside are arranged on a substrate, and pressure is measured from a change in capacitance between the diaphragm electrode and the fixed electrode opposed to the diaphragm electrode. In the vacuum sensor, a temperature control unit for controlling the temperature around the diaphragm electrode to a constant temperature is provided on the substrate on which the diaphragm electrode and the fixed electrode are arranged, and the pressure detection unit of the vacuum sensor is formed of a plurality of wires. It is a capacitance type vacuum sensor characterized by being supported. In the above,
The temperature control means is obtained by forming a heating layer and a temperature measurement layer on a substrate.
【0006】[0006]
【発明の実施の形態】本発明は、弾性隔膜(ダイヤフラ
ム電極)によって複数の領域を空間的に仕切り、前記仕
切られた領域の一つあるいは複数の領域内の圧力が変化
したとき、前記ダイヤフラム電極で仕切られた複数の部
屋内の圧力差に応じて、前記ダイヤフラム電極が変位す
るので、その変位量を前記ダイヤフラム電極に対向して
設けられた固定電極との間の静電容量の変化としてとら
え、これから圧力を測定する方式の真空センサにおい
て、前記ダイヤフラム電極および固定電極が形成されて
いる基板上に加熱手段と温度測定手段とを設置し、前記
ダイヤフラム電極および固定電極が形成されている基板
全体を加熱して温度を一定に制御し、前記ダイヤフラム
及び固定電極が形成されている基板の周辺を断熱構造に
することにより、その周辺への熱伝導を抑え、前記ダイ
ヤフラム電極及び固定電極が形成されている基板の昇温
時間の短縮化と温度制御性の向上、省電力化を行うこと
ができるように構成したことを特徴とする静電容量型真
空センサである。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention is directed to a method of the present invention wherein a plurality of regions are spatially partitioned by an elastic diaphragm (diaphragm electrode), and when the pressure in one or more of the partitioned regions changes, the diaphragm electrode is used. The diaphragm electrode is displaced in accordance with the pressure difference in the plurality of chambers partitioned by the above, and the amount of displacement is taken as a change in capacitance between the diaphragm electrode and a fixed electrode provided opposite to the diaphragm electrode. In a vacuum sensor for measuring pressure from now on, a heating unit and a temperature measuring unit are installed on a substrate on which the diaphragm electrode and the fixed electrode are formed, and the entire substrate on which the diaphragm electrode and the fixed electrode are formed. Is heated to control the temperature to be constant, and the periphery of the substrate on which the diaphragm and the fixed electrode are formed is made to have a heat insulating structure. It is characterized in that heat conduction to the periphery is suppressed, the temperature of the substrate on which the diaphragm electrode and the fixed electrode are formed is shortened, the temperature controllability is improved, and power consumption is reduced. This is a capacitance type vacuum sensor.
【0007】本発明によれば、前記昇温時間は短縮し、
温度制御性の向上によってセンサの精度を著しく向上す
ることができる。According to the present invention, the heating time is reduced,
By improving the temperature controllability, the accuracy of the sensor can be significantly improved.
【0008】[0008]
【実施例】本発明の実施例を図1に基づいて説明する。
図1にある静電容量型真空センサは、例えば半導体製造
プロセス技術を応用して作製されたものであり、圧力検
出部(主に、図中のガラス基板13とSi基板12を合
わせた構造体)の大きさは数mm〜数10mm程度、厚
さは1mm程度である。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described with reference to FIG.
The capacitance-type vacuum sensor shown in FIG. 1 is manufactured by applying, for example, a semiconductor manufacturing process technology, and includes a pressure detection unit (mainly a structure in which a glass substrate 13 and a Si substrate 12 in the figure are combined. ) Is about several mm to several tens of mm, and the thickness is about 1 mm.
【0009】図中の2は、内部の圧力測定を行う真空装
置であり、ゲージポートやフランジポート(図中17)
に本真空センサを取り付けて使用する。3は、真空装置
2に連通する領域であり、この領域の圧力は、真空装置
2の圧力にほぼ等しい。1は基準圧力室で、ダイヤフラ
ム電極14が形成されているSi基板12と固定電極1
5が形成されているガラス基板13に挾まれた領域で、
高真空圧力に封止されている。Reference numeral 2 in the figure denotes a vacuum device for measuring the internal pressure, which is a gauge port or a flange port (17 in the figure).
This vacuum sensor is attached to and used. Reference numeral 3 denotes a region communicating with the vacuum device 2, and the pressure in this region is substantially equal to the pressure of the vacuum device 2. Reference numeral 1 denotes a reference pressure chamber, and the Si substrate 12 on which the diaphragm electrode 14 is formed and the fixed electrode 1
5 is formed in a region sandwiched by the glass substrate 13 on which
Sealed to high vacuum pressure.
【0010】前記ダイヤフラム電極14は、真空装置2
に連通する領域3と接触しており、該領域3の圧力が変
化するとそれに応じて、ダイヤフラム電極14を押す力
も変化し、その変化量に応じて、ダイヤフラム電極14
とそれに対向する位置にある固定電極15との距離は変
位する。The diaphragm electrode 14 is connected to the vacuum device 2
When the pressure in the region 3 changes, the force for pressing the diaphragm electrode 14 also changes, and according to the amount of change, the diaphragm electrode 14
The distance between the fixed electrode 15 and the position facing the fixed electrode 15 is displaced.
【0011】前記ダイヤフラム電極14と固定電極15
の間に電圧を印加した場合、両電極間の静電容量は、ダ
イヤフラム電極14と固定電極15間の距離に反比例す
ることから、真空装置2の内部の圧力は、前記両電極間
の静電容量から求めることができる。The diaphragm electrode 14 and the fixed electrode 15
When a voltage is applied between the electrodes, the capacitance between the two electrodes is inversely proportional to the distance between the diaphragm electrode 14 and the fixed electrode 15, so that the pressure inside the vacuum device 2 It can be obtained from the capacity.
【0012】ここで、ダイヤフラム電極14を有するS
i基板12と、固定電極15を有するガラス基板13の
構造について説明する。Here, the S electrode having the diaphragm electrode 14
The structure of the i-substrate 12 and the glass substrate 13 having the fixed electrode 15 will be described.
【0013】前記ダイヤフラム電極14を有するSi基
板12と、固定電極15を有するガラス基板13は、そ
れぞれ、厚さ0.4mmのシリコンウェハーと厚さ1m
mのパイレックスガラス(コーニング社製)である。但
し、シリコンウェハーと同じ、あるいは非常に近い熱膨
張係数を持つガラス等の材料であれば、その限りではな
い。The Si substrate 12 having the diaphragm electrode 14 and the glass substrate 13 having the fixed electrode 15 are each composed of a silicon wafer having a thickness of 0.4 mm and a silicon wafer having a thickness of 1 m.
m Pyrex glass (manufactured by Corning Incorporated). However, the material is not limited as long as it is a material such as glass having the same or very close thermal expansion coefficient as that of the silicon wafer.
【0014】前記ダイヤフラム電極14は、通常、半導
体産業の微細加工で使用されているドライエッチング等
の技術により容易に形成される。ダイヤフラム電極14
の厚みは、5μmである。The diaphragm electrode 14 is usually easily formed by a technique such as dry etching used in fine processing in the semiconductor industry. Diaphragm electrode 14
Is 5 μm.
【0015】また、固定電極15は、通常、スパッタリ
ング、または蒸着などの真空を利用した薄膜技術によっ
て形成され、ここではA1(アルミニウム)を使用して
いる。The fixed electrode 15 is usually formed by a thin film technique utilizing a vacuum such as sputtering or vapor deposition, and here uses A1 (aluminum).
【0016】前記ダイヤフラム電極14を有するSi基
板12と、固定電極15を有するガラス基板13は、両
電極間が、7μmになるように微細加工され、陽極接合
技術により接合される。The Si substrate 12 having the diaphragm electrode 14 and the glass substrate 13 having the fixed electrode 15 are finely processed so as to have a thickness of 7 μm between the two electrodes, and are bonded by an anodic bonding technique.
【0017】次に、図中のガラス基板18上に形成され
る発熱層16、および温度測定層18について説明す
る。Next, the heat generation layer 16 and the temperature measurement layer 18 formed on the glass substrate 18 in the drawing will be described.
【0018】前記発熱層16は、例えば、ニクロム系、
タンタル系等の発熱材料からなり、スパッタリング、ま
たは蒸着等の真空を利用した薄膜技術とドライエッチン
グ等による微細加工技術によって、基板上に均一に直接
形成される。発熱層16の厚みは、約数μmであり、こ
れにより、ダイヤフラム電極14の周辺の空間は、約5
0℃〜200℃の温度範囲で加熱される。The heating layer 16 is made of, for example, a nichrome-based material.
It is made of a heat-generating material such as tantalum, and is uniformly formed directly on a substrate by a thin film technique utilizing vacuum such as sputtering or vapor deposition and a fine processing technique such as dry etching. The thickness of the heat generating layer 16 is about several μm, so that the space around the diaphragm electrode 14 is about 5 μm.
It is heated in a temperature range of 0 ° C to 200 ° C.
【0019】また発熱層16の上には、加熱温度を測定
するために、抵抗値と温度の関係を利用したSiCなど
の抵抗体、または、熱起電力と温度の関係を利用した金
属材料からなる温度測定層18が形成されている。温度
測定層18は発熱層16と同様の薄膜技術、及び微細加
工技術で形成され、導線9を介して電気回路7に出力
し、モニターできる構造をしている。前記導線9は、真
空センサを支持する支持体の役割も兼ねている。In order to measure the heating temperature, a resistor such as SiC utilizing the relationship between the resistance value and the temperature or a metal material utilizing the relationship between the thermoelectromotive force and the temperature is provided on the heating layer 16. A temperature measurement layer 18 is formed. The temperature measurement layer 18 is formed by the same thin film technology and fine processing technology as the heat generation layer 16, and has a structure that can be output to the electric circuit 7 via the conductive wire 9 and monitored. The conducting wire 9 also serves as a support for supporting the vacuum sensor.
【0020】導線9は、固定電極15、発熱層16、及
び温度測定層18に接触する各種導線があり、そのた
め、少なくても3点以上で支持されることになる。ま
た、導線9は、数ミリオーダーの長さであるため、約1
0ミリ角の圧力検出部(Si基板12とガラス基板13
の接合体)を支持するには充分の強度と振動等に対する
安定性を備える。The conductive wire 9 includes various conductive wires that come into contact with the fixed electrode 15, the heat generating layer 16, and the temperature measuring layer 18, and is therefore supported at at least three points. Further, since the length of the conductive wire 9 is several millimeters, it is approximately 1 mm.
0 mm square pressure detector (Si substrate 12 and glass substrate 13
) And have sufficient strength and stability against vibration and the like.
【0021】このような形態を採ることで、導線9を介
しての熱伝導以外に周辺構造から熱的影響を受けること
がなくなるため、真空中に隔絶した形で固定された圧力
検出部は、優れた断熱構造を有することになる。By adopting such a form, since there is no thermal influence from the surrounding structure other than the heat conduction through the conducting wire 9, the pressure detector fixed in a vacuum isolated form It will have an excellent heat insulation structure.
【0022】従って、従来型に比べ、小型で熱容量が格
段に小さい、本発明による静電容量型真空センサでは、
圧力測定が可能となる安定化時間の短縮化と温度制御性
の向上が図られる。Therefore, in the capacitance type vacuum sensor according to the present invention, which is smaller and has a much smaller heat capacity than the conventional type,
The stabilization time for enabling pressure measurement is shortened and the temperature controllability is improved.
【0023】図3は、従来型静電容量型真空センサの圧
力検出部の出力電圧の変動を示す。測定は、圧力変化の
要因を除くため、一定の減圧下で行い、加熱温度を50
℃にした。図は、本来、圧力変化が無いため、センサの
出力電圧に変動はなく、一定となるはずであるが、加熱
後、熱的要因により、センサの出力電圧が、上下変動の
振幅を狭めながらも、安定化するまで2時間以上を要し
ていることを示している。FIG. 3 shows the fluctuation of the output voltage of the pressure detector of the conventional capacitive vacuum sensor. The measurement is performed under a constant reduced pressure in order to eliminate the factor of the pressure change, and the heating temperature is set to 50
° C. The figure shows that the output voltage of the sensor should be constant and constant because there is no pressure change.However, after heating, the output voltage of the sensor is reduced due to thermal factors while reducing the amplitude of the vertical fluctuation. , It takes more than 2 hours to stabilize.
【0024】一方、本発明による静電容量型真空センサ
によれば、上記安定化時間が約1/100程度に短縮さ
れ、加熱後、約2分以内でセンサの出力電圧が一定とな
ることが確認された。On the other hand, according to the capacitance type vacuum sensor of the present invention, the stabilization time is reduced to about 1/100, and the output voltage of the sensor becomes constant within about 2 minutes after heating. confirmed.
【0025】[0025]
【発明の効果】本発明の温度制御機能付き静電容量型真
空センサによれば、大きさ数mmから数十mm程度、厚
さ1mm程度のものが実現できるので、著しく小型化し
得る効果がある。更に本発明のセンサは真空内に設置さ
れるためにセンサからの放熱は細い導線や希薄な周辺ガ
スへの熱伝導や熱輻射だけなので、優れた断熱構造とな
り、保温性にも優れているなどの諸効果がある。従って
センサ自体の熱容量も、従来の静電容量型真空センサよ
り格段に小型になる為に、省電力での加熱、昇温時間の
短縮、急激なセンサの温度変化に対する迅速なセンサ温
度制御が可能で、特別な機構によらなくても均一加熱が
できるなどの効果がある。According to the capacitive vacuum sensor with a temperature control function of the present invention, a sensor having a size of about several mm to several tens of mm and a thickness of about 1 mm can be realized. . Furthermore, since the sensor of the present invention is installed in a vacuum, heat radiation from the sensor is only heat conduction and heat radiation to a thin conductive wire or a dilute peripheral gas, so it has an excellent heat insulation structure and excellent heat retention. There are various effects. Therefore, the heat capacity of the sensor itself is much smaller than that of the conventional capacitive vacuum sensor, enabling heating with reduced power consumption, shortening the temperature rise time, and quick sensor temperature control in response to sudden sensor temperature changes. Thus, there is an effect that uniform heating can be performed without using a special mechanism.
この発明の実施例の一部を省略した説明図。従来の静電
容量型真空センサの構造の説明図。同じく出力電圧の変
動グラフ。FIG. 1 is an explanatory view in which a part of an embodiment of the present invention is omitted. FIG. 4 is an explanatory diagram of a structure of a conventional capacitance vacuum sensor. Similarly, the output voltage fluctuation graph.
1 基準圧力室 2 真空装置 3 真空装置に連通する領域 4、14 ダイヤフラム電極 5、15 固定電極 6 加熱部 7 電気回路 8 温度測定部 9 導線 10 断熱材 11 センサケース 12 Si基板 13 ガラス基板 16 加熱層 17 フランジポート 18 温度測定層 REFERENCE SIGNS LIST 1 Reference pressure chamber 2 Vacuum device 3 Area communicating with vacuum device 4, 14 Diaphragm electrode 5, 15 Fixed electrode 6 Heating unit 7 Electric circuit 8 Temperature measuring unit 9 Conductor 10 Insulation material 11 Sensor case 12 Si substrate 13 Glass substrate 16 Heating Layer 17 Flange port 18 Temperature measurement layer
─────────────────────────────────────────────────────
────────────────────────────────────────────────── ───
【手続補正書】[Procedure amendment]
【提出日】平成11年6月15日(1999.6.1
5)[Submission date] June 15, 1999 (1999.6.1
5)
【手続補正1】[Procedure amendment 1]
【補正対象書類名】明細書[Document name to be amended] Statement
【補正対象項目名】図面の簡単な説明[Correction target item name] Brief description of drawings
【補正方法】変更[Correction method] Change
【補正内容】[Correction contents]
【図面の簡単な説明】[Brief description of the drawings]
【図1】この発明の実施例の一部を省略した説明図。FIG. 1 is an explanatory view in which a part of an embodiment of the present invention is omitted.
【図2】従来の静電容量型真空センサの構造の説明図。FIG. 2 is an explanatory view of the structure of a conventional capacitance vacuum sensor.
【図3】同じく出力電圧の変動グラフ。FIG. 3 is a graph showing a variation in output voltage.
【符号の説明】 1 基準圧力室 2 真空装置 3 真空装置に連通する領域 4、14 ダイヤフラム電極 5、15 固定電極 6 加熱部 7 電気回路 8 温度測定部 9 導線 10 断熱材 11 センサケース 12 Si基板 13 ガラス基板 16 加熱層 17 フランジポート 18 温度測定層[Description of Signs] 1 Reference pressure chamber 2 Vacuum device 3 Area communicating with vacuum device 4, 14 Diaphragm electrode 5, 15 Fixed electrode 6 Heating unit 7 Electric circuit 8 Temperature measuring unit 9 Conductor 10 Heat insulating material 11 Sensor case 12 Si substrate 13 Glass substrate 16 Heating layer 17 Flange port 18 Temperature measurement layer
Claims (3)
ヤフラム電極と固定電極とを基板に配置し、前記ダイヤ
フラム電極と対向する固定電極との間の静電容量の変化
から圧力を測定する真空センサにおいて、前記ダイヤフ
ラム電極および前記固定電極が配置されている前記基板
上にダイヤフラム電極周辺を一定温度にする為の温度制
御手段を設けたことを特徴とする静電容量型真空セン
サ。1. A vacuum for arranging a pair of diaphragm electrodes and a fixed electrode facing each other with a space therebetween on a substrate, and measuring pressure from a change in capacitance between the diaphragm electrode and the fixed electrode facing the vacuum electrode. In the sensor, a capacitance type vacuum sensor is provided on the substrate on which the diaphragm electrode and the fixed electrode are disposed, for controlling the temperature around the diaphragm electrode to be constant.
ヤフラム電極と固定電極とを基板に配置し、前記ダイヤ
フラム電極と対向する固定電極との間の静電容量の変化
から圧力を測定する真空センサにおいて、前記ダイヤフ
ラム電極および前記固定電極が配置されている前記基板
上にダイヤフラム電極周辺を一定温度にする為の温度制
御手段を設けると共に、前記真空センサの圧力検出部を
複数本の線材で支持したことを特徴とする静電容量型真
空センサ。2. A vacuum in which a pair of diaphragm electrodes and a fixed electrode facing each other with a space therebetween are disposed on a substrate, and pressure is measured from a change in capacitance between the diaphragm electrode and the fixed electrode facing the vacuum electrode. In the sensor, a temperature control unit is provided on the substrate on which the diaphragm electrode and the fixed electrode are arranged to maintain a constant temperature around the diaphragm electrode, and a pressure detecting unit of the vacuum sensor is supported by a plurality of wires. A capacitance type vacuum sensor characterized in that:
測定層を形成したことを特徴とする請求項1又は2記載
の静電容量型真空センサ。3. The capacitance type vacuum sensor according to claim 1, wherein the temperature control means has a heat generating layer and a temperature measuring layer formed on the substrate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13413699A JP4437336B2 (en) | 1999-05-14 | 1999-05-14 | Capacitive vacuum sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13413699A JP4437336B2 (en) | 1999-05-14 | 1999-05-14 | Capacitive vacuum sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JP2000321161A true JP2000321161A (en) | 2000-11-24 |
| JP4437336B2 JP4437336B2 (en) | 2010-03-24 |
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ID=15121322
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13413699A Expired - Fee Related JP4437336B2 (en) | 1999-05-14 | 1999-05-14 | Capacitive vacuum sensor |
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| Country | Link |
|---|---|
| JP (1) | JP4437336B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI452275B (en) * | 2005-08-12 | 2014-09-11 | Inficon Gmbh | Vacuum measuring cell |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7140925B2 (en) * | 2019-02-26 | 2022-09-21 | スミトモ (エスエイチアイ) クライオジェニックス オブ アメリカ インコーポレイテッド | Thermal barrier between electronics and high temperature sensors in capacitive diaphragm gauges |
| WO2023101715A1 (en) | 2021-12-03 | 2023-06-08 | Sumitomo (Shi) Cryogenics Of America, Inc. | Thermal insulation system for a capacitance diaphragm gauge |
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1999
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|---|---|---|---|---|
| JPS5596589A (en) * | 1979-01-18 | 1980-07-22 | Toray Industries | Panel heater |
| JPS6332333A (en) * | 1985-08-08 | 1988-02-12 | ロ−ベルト・ボツシユ・ゲゼルシヤフト・ミツト・ベシユレンクテル・ハフツング | Pressure measuring can |
| JPS62182636A (en) * | 1986-02-06 | 1987-08-11 | Anelva Corp | Diaphragm type vacuum gauge |
| JPH01102841U (en) * | 1987-12-28 | 1989-07-11 | ||
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| JPH0495740A (en) * | 1990-08-06 | 1992-03-27 | Toyota Autom Loom Works Ltd | Semiconductor device |
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| JPH0943079A (en) * | 1995-07-27 | 1997-02-14 | Matsushita Electric Ind Co Ltd | Capacitive pressure sensor and gas abnormality monitoring device using this sensor |
| JPH09126920A (en) * | 1995-10-26 | 1997-05-16 | Matsushita Electric Works Ltd | Semiconductor pressure sensor |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI452275B (en) * | 2005-08-12 | 2014-09-11 | Inficon Gmbh | Vacuum measuring cell |
Also Published As
| Publication number | Publication date |
|---|---|
| JP4437336B2 (en) | 2010-03-24 |
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